Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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3296 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6\phi_1q_2\tilde{q}_2$ | 0.6477 | 0.8502 | 0.7618 | [X:[], M:[1.0, 1.0405, 0.919, 0.7601, 0.7196, 0.7196], q:[0.7601, 0.2399], qb:[0.5203, 0.5608], phi:[0.4797]] | [X:[], M:[[0], [4], [-8], [1], [-3], [-3]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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$M_5$, $ M_6$, $ M_4$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ M_3$, $ \phi_1q_2^2$, $ M_1$, $ M_2$, $ q_1\tilde{q}_2$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ M_4M_5$, $ M_4M_6$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_4^2$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ M_5q_2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_3M_5$, $ M_3M_6$, $ M_3M_4$, $ M_5\phi_1q_2^2$, $ M_6\phi_1q_2^2$, $ M_1M_5$, $ M_1M_6$, $ M_4\phi_1q_2^2$, $ \phi_1q_2^3\tilde{q}_1$, $ M_1M_4$, $ M_2M_5$, $ M_2M_6$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_2$, $ M_2M_4$, $ M_2q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$, $ M_3^2$, $ M_2q_2\tilde{q}_2$, $ M_3\phi_1q_2^2$, $ M_1M_3$, $ \phi_1^2q_2^4$ | . | -2 | 2*t^2.16 + 2*t^2.28 + t^2.4 + t^2.76 + t^2.88 + t^3. + t^3.12 + t^3.96 + 3*t^4.32 + 4*t^4.44 + 6*t^4.56 + 3*t^4.68 + 2*t^4.8 + 2*t^4.92 + 3*t^5.04 + 4*t^5.16 + 5*t^5.28 + 3*t^5.4 + t^5.51 + t^5.52 + t^5.64 + 2*t^5.76 - 2*t^6. + t^6.12 + 2*t^6.24 + t^6.36 + 3*t^6.48 + 4*t^6.6 + 9*t^6.72 + 9*t^6.84 + 8*t^6.96 + 3*t^7.07 + 5*t^7.08 + 5*t^7.2 + 2*t^7.21 + 8*t^7.32 + 10*t^7.44 + 9*t^7.56 + 2*t^7.67 + 7*t^7.68 + 3*t^7.79 + 3*t^7.8 + 5*t^7.92 + 2*t^7.93 + 3*t^8.04 - 4*t^8.16 + t^8.27 - 5*t^8.28 + t^8.39 - 3*t^8.4 + 2*t^8.51 + 2*t^8.52 + 7*t^8.64 + t^8.76 + 2*t^8.77 + 6*t^8.88 - t^4.44/y - (2*t^6.6)/y - t^6.72/y - t^7.2/y + t^7.32/y + (4*t^7.44)/y + (3*t^7.56)/y + (3*t^7.68)/y + (2*t^7.92)/y + (4*t^8.04)/y + (6*t^8.16)/y + (7*t^8.28)/y + (3*t^8.4)/y + t^8.52/y + t^8.64/y - (2*t^8.76)/y - t^4.44*y - 2*t^6.6*y - t^6.72*y - t^7.2*y + t^7.32*y + 4*t^7.44*y + 3*t^7.56*y + 3*t^7.68*y + 2*t^7.92*y + 4*t^8.04*y + 6*t^8.16*y + 7*t^8.28*y + 3*t^8.4*y + t^8.52*y + t^8.64*y - 2*t^8.76*y | (2*t^2.16)/g1^3 + 2*g1*t^2.28 + g1^5*t^2.4 + t^2.76/g1^8 + t^2.88/g1^4 + t^3. + g1^4*t^3.12 + g1^7*t^3.96 + (3*t^4.32)/g1^6 + (4*t^4.44)/g1^2 + 6*g1^2*t^4.56 + 3*g1^6*t^4.68 + 2*g1^10*t^4.8 + (2*t^4.92)/g1^11 + (3*t^5.04)/g1^7 + (4*t^5.16)/g1^3 + 5*g1*t^5.28 + 3*g1^5*t^5.4 + t^5.51/g1^16 + g1^9*t^5.52 + t^5.64/g1^12 + (2*t^5.76)/g1^8 - 2*t^6. + g1^4*t^6.12 + 2*g1^8*t^6.24 + g1^12*t^6.36 + (3*t^6.48)/g1^9 + (4*t^6.6)/g1^5 + (9*t^6.72)/g1 + 9*g1^3*t^6.84 + 8*g1^7*t^6.96 + (3*t^7.07)/g1^14 + 5*g1^11*t^7.08 + (5*t^7.2)/g1^10 + 2*g1^15*t^7.21 + (8*t^7.32)/g1^6 + (10*t^7.44)/g1^2 + 9*g1^2*t^7.56 + (2*t^7.67)/g1^19 + 7*g1^6*t^7.68 + (3*t^7.79)/g1^15 + 3*g1^10*t^7.8 + (5*t^7.92)/g1^11 + 2*g1^14*t^7.93 + (3*t^8.04)/g1^7 - (4*t^8.16)/g1^3 + t^8.27/g1^24 - 5*g1*t^8.28 + t^8.39/g1^20 - 3*g1^5*t^8.4 + (2*t^8.51)/g1^16 + 2*g1^9*t^8.52 + (5*t^8.64)/g1^12 + 2*g1^13*t^8.64 + t^8.76/g1^8 + 2*g1^17*t^8.77 + (6*t^8.88)/g1^4 - t^4.44/(g1^2*y) - (2*t^6.6)/(g1^5*y) - t^6.72/(g1*y) - t^7.2/(g1^10*y) + t^7.32/(g1^6*y) + (4*t^7.44)/(g1^2*y) + (3*g1^2*t^7.56)/y + (3*g1^6*t^7.68)/y + (2*t^7.92)/(g1^11*y) + (4*t^8.04)/(g1^7*y) + (6*t^8.16)/(g1^3*y) + (7*g1*t^8.28)/y + (3*g1^5*t^8.4)/y + (g1^9*t^8.52)/y + t^8.64/(g1^12*y) - (2*t^8.76)/(g1^8*y) - (t^4.44*y)/g1^2 - (2*t^6.6*y)/g1^5 - (t^6.72*y)/g1 - (t^7.2*y)/g1^10 + (t^7.32*y)/g1^6 + (4*t^7.44*y)/g1^2 + 3*g1^2*t^7.56*y + 3*g1^6*t^7.68*y + (2*t^7.92*y)/g1^11 + (4*t^8.04*y)/g1^7 + (6*t^8.16*y)/g1^3 + 7*g1*t^8.28*y + 3*g1^5*t^8.4*y + g1^9*t^8.52*y + (t^8.64*y)/g1^12 - (2*t^8.76*y)/g1^8 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
2780 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_4\phi_1q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ | 0.6276 | 0.8128 | 0.7721 | [X:[], M:[1.0, 1.0367, 0.9266, 0.7592, 0.7225], q:[0.7592, 0.2408], qb:[0.5183, 0.555], phi:[0.4817]] | t^2.17 + 2*t^2.28 + t^2.39 + t^2.78 + t^2.89 + t^3. + t^3.11 + t^3.83 + t^3.94 + t^4.33 + 2*t^4.44 + 5*t^4.56 + 3*t^4.67 + 2*t^4.78 + t^4.95 + 2*t^5.06 + 3*t^5.17 + 4*t^5.28 + 3*t^5.39 + t^5.5 + t^5.56 + t^5.67 + 2*t^5.78 - t^6. - t^4.44/y - t^4.44*y | detail |